Geometric factors affecting the enhanced electrocatalysis on nanoporous Pt (L2-ePt) were examined by electrochemical methods and computer simulations. The experimental results revealed that the electrochemical enhancement of O2 and H2O2 does not come only from expansion of the active surface area (so-called roughness factor, f R) of L2-ePt. The presence of extra contribution was verified by the fact that significant enhancement in electrocatalytic reactions remained even after the effect of the f R was eliminated from the electrochemical redox behavior of O2 and H2O2 on L2-ePt electrodes. Not only the voltammetric observation but also potentiometric pH responses of L2-ePt suggested the presence of unique nanoporous effects other than the surface enlargement in regard to heterogeneous electrochemical reactions. L2-ePt showed near Nernstian behavior, faster response time, and less hysteresis even if the real surface area was smaller than that of flat Pt. Increased residence time near the electrode surface due to extremely confined space of nanoporous structure was proposed as possible origins and examined by the Monte Carlo simulations of simple model electrodes. The theoretical approaches indicated that long residence time of reactant at electrode surface by confinement effect of the nanoporous environment well accounted for the experimental results.

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In this study, we investigated the pure geometrical effect of porous materials in gas adsorption using the grand canonical Monte Carlo simulations of primitive gas-pore models with various pore geometries such as planar, cylindrical, and random pore geometries. Although the model does not possess atomistic level details of porous materials, our simulation results provided many insightful information in the effect of pore geometry on the adsorption behavior of gas molecules. First, the surface curvature of porous materials plays a significant role in the amount of adsorbed gas molecules: the concave surface such as in cylindrical pores induces more attraction between gas molecules and pore, which results in the enhanced gas adsorption. On the contrary, the convex surface of random pores gives the opposite effect. Second, this geometrical effect shows a nonmonotonic dependence on the gas-pore interaction strength and length. Third, as the external gas pressure is increased, the change in the gas adsorption due to pore geometry is reduced. Finally, the pore geometry also affects the collision dynamics of gas molecules. Since our model is based on primitive description of fluid molecules, our conclusion can be applied to any fluidic systems including reactant-electrode systems.